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The nonlinear model was numerically solved with the implicit, finite difference approximation using the Newton-Raphson's method [26].
The reservoir model was numerically constructed using 100 grid blocks in the radial direction and 20 grid blocks in the vertical direction.
The model was numerically implemented in analogy to incremental plasticity and successfully applied for finite-element (FE) simulations of nanoindentation.
The model was numerically calculated based on the modified SIMPLE algorithm, and the height of cuttings bed was predicted by the trial-and-error method.
The total response of the proposed model was numerically simulated as shown in Fig. 4, in comparison with the experimentally measured results which were obtained in the same setup as in [16].
Breakage of agglomerates above a bubble as assumed in the development of the Iwadate and Horio (Powder Technol. 100 (1998a) 223) model (I H model) was numerically confirmed.
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The model is numerically simulated and validated using the available experimental and numerical data.
The proposed model is numerically implemented.
Finally, the analytical model is numerically and experimentally validated.
The random-anisotropy Heisenberg model is numerically studied on lattices containing over ten million spins.
The derived model is numerically solved using Chebyshev spectral collocation method.
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